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United States Patent |
5,336,963
|
Haga
,   et al.
|
August 9, 1994
|
Color cathode-ray tube
Abstract
In a color cathode-ray tube having a shadow mask disposed to face a
phosphor screen and having apertures for passage of an electron beam, and
a frame for reinforcing tile periphery of the shadow mask, a magnetic
shield comprises strips of magnetic material each having a first end fixed
to the frame and a second end disposed closer to the electron gun. Because
of the elongated shape, the strips are magnetized easily only in the
direction of their length. As a result, an external magnetic field
parallel to the strips, and hence with the tube axis, is reduced or
canceled. Moreover, if each strip is bent near its second end so that the
second end is directed toward a horizontal plane containing the tube axis,
an external magnetic field in the direction in which the second end is
directed is enhanced. This will further reduce deviation of the electron
beam path In the horizontal direction.
Inventors:
|
Haga; Akira (Sendai, JP);
Nasuno; Hiroshi (Kurihara, JP);
Fujimura; Takeo (Nagaokakyo, JP)
|
Assignee:
|
Mitsubishi Denki Kabushiki Kaisha (Tokyo, JP);
Tohoku Gakuin University (Sendai, JP)
|
Appl. No.:
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140711 |
Filed:
|
October 22, 1993 |
Foreign Application Priority Data
Current U.S. Class: |
313/402; 313/407 |
Intern'l Class: |
H01J 029/07 |
Field of Search: |
313/402,407
|
References Cited
U.S. Patent Documents
4019085 | Apr., 1977 | Sakata | 313/407.
|
4229675 | Oct., 1980 | Matsuki et al. | 313/402.
|
4385256 | May., 1983 | Tokita et al. | 313/407.
|
4580076 | Apr., 1986 | Shimoma et al. | 313/402.
|
4858016 | Aug., 1989 | Suehiro et al. | 358/246.
|
Foreign Patent Documents |
0217473 | Apr., 1987 | EP.
| |
0403010 | Dec., 1990 | EP.
| |
3807125 | Sep., 1988 | DE.
| |
Primary Examiner: O'Shea; Sandra L.
Parent Case Text
This application is a continuation, of application Ser. No. 07,892,589
filed on Jun. 3, 1992, which is now abandoned.
Claims
What is claimed is:
1. A color cathode-ray tube comprising:
an envelope having a generally rectangular front panel;
a phosphor screen provided on an inner surface of said front panel;
a shadow mask positioned to face said phosphor screen and having apertures
for passage of an electron beam;
an electron gun positioned to face the phosphor screen and emitting an
electron beam toward the shadow mask;
a frame for reinforcing the periphery of the shadow mask and fixing the
shadow mask with respect to the inner surface of said front panel; and
a magnetic shield comprising a plurality of strips of a magnetic material
each of the strips having a first end fixed to said frame and a second end
disposed closer to said electron gun;
wherein said second end of each of the strips is not in contact with a
high-permeability magnetic member.
2. The tube of claim 1, wherein said strip is made of a high-permeability
material, and having a ratio of its length to its thickness of not less
than 5 and a ratio of its length to its width of not less than 2.
3. The tube of claim 1, wherein said strip is substantially straight and is
inclined with respect to a plane containing an edge of the frame and
parallel with an axis of the tube.
4. The tube of claim 3, wherein said strip extends along the inner surface
of the funnel.
5. The tube of claim 1, wherein said strip has a trunk part having one end
fixed to said frame and extending from the first part toward said electron
gun, and a tip part coupled to the trunk part and having a tip directed
toward a plane containing an axis of the tube and an axis perpendicular to
the said axis of the tube and parallel to longer sides of the front panel.
6. The tube of claim 5, wherein said trunk part and said tip part are
continuous and formed by bending a continuous strip.
7. The tube of claim 1, wherein said magnetic shield comprises a plurality
of said strips.
8. The tube of claim 7, wherein the second ends of said the strips are
connected together by means of a non-magnetic connecting member and are
thereby reinforced.
9. The tube of claim 7, wherein said magnetic shield further comprises a
connecting part extending along the side wall of the frame, and fixed to
the frame, and the first ends of said strips are connected to said
connecting part.
10. The tube of claim 7, wherein the frame is of a rectangular shape and
there are at least two of said strips in physical contact with each of
said walls.
11. The tube of claim 10 wherein there are a total of 34 strips and each of
said strips are spaced from each other at an equal interval of 1 cm.
12. A color cathode-ray tube comprising:
an envelope having a generally rectangular front panel;
a phosphor screen provided on an inner surface of said front panel;
a shadow mask positioned to face said phosphor screen and having apertures
for passage of an electron beam;
an electron gun positioned to face the phosphor screen and emitting an
electron beam toward the shadow mask;
a frame for reinforcing the periphery of the shadow mask and fixing the
shadow mask with respect to the inner surface of said front panel, said
frame having a rectangular shape and having a top, bottom and side walls,
a one piece monolithic magnetic shield comprising a connection part in
direct physical contact with the frame and a plurality of strip parts
common to and extending beyond the frame in the direction of said electron
gun from the connection part wherein a tip part of each of said strips is
not in contact with a high-permeability magnetic member.
13. The tube of claim 12 wherein the strip parts have a curved tip part
remote from said connecting part.
14. The tube of claim 12 wherein said strip parts are bent adjacent to said
connecting part to form an angle of inclination with the wall to which the
connecting part is attached.
15. The tube of claim 12 wherein there are a total of 34 strips.
16. The tube of claim 13 wherein there are a total of 34 strips.
17. The tube of claim 14 wherein there are a total of 34 strips.
18. The tube of claim 1, wherein said plurality of strips are disposed on
top and bottom sides of the frame.
19. A color cathode-ray tube comprising:
an envelope having a generally rectangular front panel;
a phosphor screen provided on an inner surface of said front panel;
a shadow mask disposed to face said phosphor screen and having apertures
for passage of an electron beam;
an electron gun disposed to face the phosphor screen and emitting an
electron beam toward the shadow mask;
a frame having four walls for reinforcing the periphery of the shadow mask
and fixing the shadow mask with respect to the inner surface of said front
panel; and
a magnetic shield comprising at least one strip of a magnetic material
having a first end fixed to and in physical contact with a wall of said
frame and a second end disposed closer to said electron gun, the strip
having a length and width, the width of the strip being substantially less
than a major length of the wall of the frame to which it is attached, so
that a plurality of strips can be attached to each of said walls.
20. The tube of claim 19, wherein there are a plurality of strips in
contact with each of the walls of the frame.
Description
BACKGROUND OF THE INVENTION
The present invention relates to a color cathode ray tube of the shadow
mask type that has a magnetic shield for preventing for example color
contamination due to deviation of the electron beam caused by an external
magnetic field such as terrestrial magnetism.
In a color cathode ray tube with a built-in shadow mask, when the electron
beam deviates under the influence of an external magnetic field, such as
terrestrial magnetism, color contamination or other undesirable phenomenon
occurs because undesired parts of a phosphor screen is made to emit light.
To eliminate the effect of the external magnetic field, an internal
magnetic shield is mounted along the inner wall of a funnel, adjacent the
edges of a generally rectangular shadow mask.
FIG. 11 is a sectional view of such a color cathode ray tube in the prior
art. In describing the color cathode ray tube, the term "Z-axis" is used
to mean the tube axis which is perpendicular to the shadow mask and
passing the center of the shadow mask, the term "X-axis" is used to mean
the axis orthogonal to the Z-axis and parallel to the longer sides
(horizontally extending sides, i.e., the top and the bottom sides) of the
shadow mask, and the term "Y-axis" is used to mean the axis orthogonal to
the Z-axis and the X-axis and parallel to the shorter sides (vertically
extending sides , i.e., the right and the left sides) of the shadow mask.
Moreover, the term "front" is used to mean the direction toward the face
plate of the cathode ray tube, and the term "rear" is used to mean the
direction toward the electron gun.
The cathode ray tube shown in FIG. 11 comprises a glass envelope 1 made up
of a neck 1a, a funnel 1b and a face plate or front panel 1c. An electron
gun 2 is disposed in the neck 1a, a phosphor screen 3 formed of phosphors
emitting light of red, green and blue are provided on the inner surface of
the front panel 1c in a mosaic fashion. A rectangular shadow mask 4 is
disposed to face the phosphor screen 3, and is provided with apertures 6
for passage of electron beams 9, as shown in FIG. 12.
A rectangular frame 5 comprises a parallel part 5a and a normal part 5b.
The parallel part 5a is flat, parallel with a skirt 1ca of the Front panel
1c and extends along the edges of the phosphor screen 3. The normal part
5b is flat, connected to the rear edge of the parallel part 5a (that side
of the parallel part 5a which is facing the electron gun 2) and extends
therefrom inward, normal to the axis, denoted by Z, of the tube 1.
The cross section of the rectangular frame 5 is therefore L-shaped.
The parallel part 5a has a width smaller than the dimension of the skirt
1ca in the direction of the tube axis Z so that it is accommodated in the
skirt 1ca.
The edges of the shadow mask 4 are fixed, by means of welding or the like,
to the sides 5a of the frame 5, so that the shadow mask 4 is reinforced.
Springs 7 have one end fixed to the parallel part 5a of the frame 5. The
shadow mask 4, the frame 5 and the springs 7 together form a shadow mask
structure 20.
The springs 7 have holes at their other ends engaged with pins (not shown)
erected on the inner surface of the respective sides of the skirt 1ca, and
the shadow mask 4 and the phosphor screen 3 face each other, being
separated by a predetermined distance.
An inner magnetic shield 8 is formed from a thin sheet and formed to have a
shape of a frustum of pyramid or prismold having side surfaces extending
along the inner surface of the funnel 1b.
The periphery 8a of the front edge of the inner magnetic shield 8 are
fixed, by means of welding or the like, to the rear side of the normal
part 5b of the frame 5.
The electron beam 9 emitted from the electron gun 2 is scanned over the
range indicated by chain lines 9a and 9b in FIG. 11, and the electron beam
having passed the apertures 6 impinges on the phosphor screen 3 to cause
selective light emission from the phosphors.
When the color cathode ray tube is in an environmental magnetic field, such
as terrestrial magnetism, the path of the electron beam 9 is bent. Such
influence of the environmental magnetic field is removed or suppressed by
the inner magnetic shield 8. That is, in the space enclosed by the inner
magnetic shield 8, the environmental magnetic field is reduced, so the
bending of the path of the electron beam 9 is reduced, and the deviation
in the position of impingement onto the phosphor screen 3 is reduced, and
the color contamination is therefore reduced.
Observation of the magnetic shielding effect of the inner magnetic shield 8
reveals that when the color cathode ray tube is disposed to face the east
or the west (disposed in the E direction or the W direction), the magnetic
flux concentrates on the inner magnetic shield 8 and the frame 5, so the
shield effect in the space within enclosed by these members is
substantial.
When the color cathode ray tube is disposed to face the north or the south
(disposed in the N direction or the S direction), the inner magnetic
shield 8 is open in the direction of the phosphor screen 3, so the
magnetic shield effect is less than when the cathode ray tube is in the E
or W direction. Thus, the magnetic shielding effect is different between
the E and W direction and N and S directions. In other words, the magnetic
shielding effect has an anisotropy. It Is however desirable that the
magnetic shielding effect is approximately equal in all directions.
However, with the magnetic shield 8 in the shape of the frustum of
pyramid, it is not possible to independently adjust the magnetic shield
effect in the E and W directions, and the N and S directions, and the
designing is made based on experience.
When the inner magnetic shield is not provided, the bending of the electron
beam path due to the environmental magnetic field when the cathode ray
tube is in the E or W direction is in the vertical direction. So, with a
type of cathode ray tube having phosphor stripes elongated in vertical
direction, the deviation of the electron beam impinging positions in the
vertical direction do not cause serious color contamination. When however
the magnetic shield 8 in the shape of a frustum of pyramid as shown in
FIG. 11 is used (to improve the shield effect for the cathode ray tube in
the N or S direction), if the cathode ray tube is in the E or W direction,
the magnetic shield 8 not only gives the desired shielding effect, but
also modifies the environmental magnetic field. The shield effect for the
cathode ray tube in the E or W direction may therefore be inferior than if
the magnetic shield 8 is not used at all. It often happens that the
intended improvement in the magnetic shielding is not attained.
The terrestrial magnetism as an environmental magnetic field consists of a
horizontal components and a vertical components, and the effect of
vertical component is constant regardless of the direction in which the
cathode ray tube is disposed. The vertical component is substantially
constant throughout a substantial part of the world, so the effect of the
vertical component can be easily eliminated by appropriate design. The
effect of the horizontal component of the terrestrial magnetism is more
difficult to overcome.
Since the prior art color cathode ray tube is configured as described
above, the shielding effect by means of the magnetic shield is
insufficient, and it is not possible to determine or alter the shielding
effect independently for the E and W directions, and for the N and S
directions. Moreover, the designing was made by experience, and was
time-consuming.
SUMMARY OF THE INVENTION
An object of the invention is to provide a color cathode ray tube utilizing
the effects of the elongated shape of the magnetic body thereby to reduce
the amount of miss-landing or deviation in the position of the impingement
of the electron beam that is due to the external magnetic field in one
direction, and that can be designed with ease.
A color cathode ray tube according to the invention comprises:
an envelope having a generally rectangular front panel;
a phosphor screen provided on an inner surface of said front panel;
an electron gun disposed to face the phosphor screen and emitting an
electron beam toward the shadow mask;
a shadow mask disposed to face said phosphor screen and having apertures
for passage of an electron beam;
a frame for reinforcing the periphery of the shadow mask and fixing the
shadow mask with respect to the inner surface of said front panel; and
a magnetic shield comprising a strip of a magnetic material having a first
end fixed to said frame and a second end disposed closer to said electron
gun.
Because of the elongated shape, the strip is magnetized easily only in the
direction of its length, so an external magnetic field in the direction
parallel to the length of the strip is reduced or canceled, while an
external magnetic field normal to the length of the strip is not affected.
In other words, the shielding effect is attained when the external
magnetic field is parallel to the length of the strip, while there is no
adverse effect when the external magnetic field in the direction normal to
the length of the strip.
By bending the second end of the strip so that its tip is directed to a
plane containing the tube axis and parallel to the longer sides of the
shadow mask, an external magnetic field in the direction normal to said
plane is enhanced, and the deviation in the electron beam path is further
reduced.
The effect of the elongated shape of the strips is better exhibited by
determining the length, thickness and width as set forth above.
By fixing the magnetic shield such that it is inclined with respect to the
frame and by forming the magnetic shield into a strip shape which does not
have any bent part in the middle, the strip of the magnetic shield can be
accommodated even when the space between the inner surface of the funnel
of the tube and the range over which the electron beam is deflected is
limited, without interfering with the path of the electron beam. With this
structure, the desired effect of the elongated shape is obtained.
By connecting the tips of a plurality of magnetic shields by means of a
non-magnetic member, the mechanical strength of the tips is increased, and
vibration and deformation due to contact with other bodies by impact or
during manufacture can be prevented.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a perspective view showing a pertinent portion of the cathode ray
tube of an embodiment of the invention.
FIG. 1A is an enlarged sectional view of part 1A in FIG. 1.
FIG. 2 is a perspective view showing a pertinent portion of the cathode ray
tube of another embodiment.
FIG. 3 is a perspective view showing a pertinent portion of the cathode ray
tube of a further embodiment.
FIG. 3A is an enlarged sectional view of part 3A in FIG. 3.
FIG. 4 is a perspective view showing a pertinent portion of the cathode ray
tube of a further embodiment.
FIG. 5 is a perspective view showing a shadow mask and a frame.
FIG. 6 is a graph which shows results of measurements of magnetic flux
density distribution that are obtained when an external magnetic field is
applied in the longitudinal direction of the strips.
FIG. 7A to FIG. 7D are diagrams for explaining the effect of the shape of
the magnetic body.
FIG. 8A to FIG. 8C are diagrams which show, by vector representation,
distribution of magnetization obtained as a result of calculation by means
of an integral equation method, on the assumption that an external
magnetic field is applied at different angles with respect to the
longitudinal direction of an elongated magnetic body.
FIG. 9A to FIG. 9C are diagrams showing magnetic fields around tips of an
elongated magnetic body magnetized in their longitudinal direction.
FIG.10 is a graph which shows results of measurements of magnetic flux
density distribution that results when an external magnetic field is
applied in the lateral direction of the strips.
FIG. 11 is a sectional view showing a cathode ray tube in the prior art.
FIG. 12 is an enlarged view showing phosphor stripes and apertures in a
shadow mask.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
Embodiments of the invention will now be described with reference to the
drawings.
FIG. 1 shows a pertinent portion of an embodiment of the invention. FIG. 1A
shows, in enlarged cross section, part 1A in FIG. 1. The cathode ray tube
of this embodiment is a 20-inch color cathode ray tube, and its general
configuration is similar to that shown in and described with reference to
FIG. 11. In FIG. 1 and FIG. 1A, members or parts identical to those in
FIG. 11 are denoted by identical reference numerals. A distinction of this
embodiment from the prior-art cathode ray tube of FIG. 11 is that it
comprises a magnetic shield MS consisting of a plurality of strips 10,
details of which will be described later.
The shadow mask 4 is provided with a multitude of elongated apertures 6
each extending in the Y axis direction, as is shown in FIG. 12.
The magnetic shield MS comprises 34 strips in all, 17 strips along each of
the longer sides, i.e., the top and the bottom sides of the frame 5, at an
equal interval of 1 cm.
Part only of the strips 10 along the top side 5c are illustrated:
illustration of others is omitted as they are formed and mounted in a
similar manner.
Each of the strips 10 is substantially J-shaped, and is conveniently formed
from a continues strip but may be considered to be composed of a root part
10r, a trunk part 10s and a curved tip part 10t, for the purpose of
explanation. The root part 10r is fixed to the top side 5c of the frame 5.
The trunk part 10s is continuous to the rear end (the end toward the
electron gun 2) of the root part 10r, and extends rearward (i.e., toward
the electron gun 2) in parallel with the Z-axis.
The tip part 10t continues to the rear end of the trunk part 10s and bent
so that the tip or free end 10a of the strip 10 is directed toward the X-Z
plane (where Y=0).
As an example, the thickness t of the strip 10 is 0.1 cm and its width b
is 1 cm. The total length l of the trunk part 10s and the tip part 10t is
10 cm, as indicated in FIG. 1 and FIG. 1A. The length of the tip part 10t
is about 1/3 of the length of the trunk part 10s.
The tip 10a of the tip part 10t is not magnetically connected to any other
high-permeability material.
The strips 10 should be formed of a magnetic material having as high a
permeability as possible, and as little residual magnetism as possible,
ideally no residual magnetism.
Let us first assume that the cathode ray tube is disposed in the N or S
direction, that is the external magnetic field is parallel with the Z
axis. The strips 10 are magnetized along their length, and the magnetized
strips create an induced magnetic field around them. The induced magnetic
field near the tip of each strip is toward or away from the tip. The
principal component of such a magnetic field around the tip part 10t is in
the direction in which the tip 10a is directed, i.e., in the Y axis
direction. The magnetization of the strips 10 therefore enhance the
magnetic field or the magnetic field component in the Y direction.
On the side of each strip, the direction of the induced nagnetic field is
opposite to the external magnetic field. Accordingly, in the region where
the electron beam would pass, which is surrounded by the strips 10, the
magnetic field induced by the magnetized strips is in the direction
opposite to the external magnetic field, and the induced magnetic field
and the external magnetic field cancel each other, at least partially. In
this way, the magnetic field in the Z axis direction is reduced, and a
magnetic shielding effect is exhibited.
Further explanation is given with reference to the results of experiments.
In FIG. 12, the phosphor screen 3 in the form of stripes comprises blue
phosphor array B, red phosphor array B and green phosphor array G, and the
electron beam apertures 6 formed in the shadow mask 4 are formed to
correspond to the phosphor arrays B, R and G. The electron beam 9 emitted
From the electron gun 2 passes the apertures 6 and impinges on the
phosphors B, R or G to cause emission of light of the desired color.
In a color cathode ray tube having a stripe-type phosphor screen 3, when
the electron beam 9 deviates in the Y direction under the influence of the
terrestrial magnetism, the electron beam 9 will impinge on the phosphor of
the same color, so the color impurity is not degraded. However, when the
electron beam 9 deviates In the X direction under the influence of the
Lorenz's force caused by the external magnetic field such as terrestrial
magnetism, the electron beam may impinge partly or entirely on an area
outside the phosphor of the desired color. This result in color
contamination. The Lorenz's force F exerted on the electrons moving at a
speed V in the magnetic field of the flux density B is given by:
F=-e(V.times.B) (1)
In the above equation, "-e" represents the electric charge of an electron,
V is a vector notation of the velocity of the electron, and B is a vector
notation of the magnetic flux density in the region where the electron
travels.
The X direction component of the Lorenz's force (component in the X axis)
Fx is given by:
Fx=-e(Vy.multidot.BZ-Vz.multidot.By) (2)
In the above equation, Vy and Vz are components of the velocity V in the Y
and Z directions, and By and Bz are components of the magnetic flux
density B in the Y and Z directions. As Fx is made smaller, the deviation
of the electron beam in the X direction is reduced, and the color
contamination is reduced.
FIG. 6 shows the results of measurement of magnetic flux densities obtained
by forming a situation simulating an actual cathode ray tube having a
diagonal size of 20 inches. That is, the shadow mask 4 and the frame 5 are
disposed at the same relative position as in a completed cathode ray tube.
For assessing the effect of the magnetic shield some of the measurements
were carried out without the magnetic shield MS, while other measurements
were carried out with the magnetic shield MS provided.
The magnetic flux density is measured at various positions along the
electron beam trajectory within a space in a cathode ray tube. The
position in FIG. 6 indicates the distance in the Z direction from a
deflection center DC (FIG. 11). The deflection center DC is a point from
which the electron beam 9 appears to fan out as seen from outside the
region where the deflection takes place. The deflection is caused by the
use of deflection coils (not shown). A magnetic field corresponding to an
environmental magnetic field of 1.0 oersted (the magnetic flux density
being 1.0 gauss) in the Z direction is applied (while the effect of the
terrestrial magnetism in the X and Y directions is removed). This can be
achieved by placing the entire system in a space about which a Helmholtz
coil is wound, and passing an electric current through the coil to
generate a magnetic field in the coil.
The actual terrestrial magnetism is on the order of 0.5 oersted, but for
the purpose of improving the measurement accuracy (i.e., for enlarging the
miss-landing to thereby facilitate the measurement), a larger value (1.0
oersted) is used.
Blank circles, triangles, and inverted triangles indicates the magnetic
flux density components Bx, By and Bz in the X, Y and Z directions that
are obtained when the magnetic shield MS is not provided as shown in FIG.
5.
In FIG. 6, in the region from the deflection center (DC where Z=0) to a
point Z=200 mm, the magnetic flux consists mainly of the Z-axis component
Bz. In the region closer to the shadow mask 4, the Z-axis component Bz is
reduced, and Y-axis and X-axis components By and Bx are increased. On the
whole, Bz>>By and the Lorenz's force in the X direction is dominating.
Calculation of the path of the beam 9 of electrons moving in a magnetic
field of such a distribution indicates that the miss-landing amount at the
corner part of the phosphor screen 3 is 147 .mu.m. If the external
magnetic field is 0.5 oersted, i.e., half the magnetic field used for time
experiment, the miss-landing is 147/2=73.5.mu., which is completely out of
the intended phosphor stripe. In order to reduce the Lorenz's force
component Fx, time magnetic field should be so modified that Bz and By are
approximately equal to each other, as will be understood from time
equation (2). In other words, Bz should be decreased, and By should be
increased. Moreover, as the polarity (sign "+" or "-") of Vy is opposite
between the upper half and time lower half of the tube, the polarity of By
should be opposite.
When a ferromagnetic body is magnetized by an external magnetic field, the
magnetization depends largely on the shape of the ferromagnetic body. For
instance, FIG. 7A to FIG. 7D are vector representation of the distribution
of magnetization of a flat magnetic body resulting from application of an
external magnetic field He at an angle of .theta.=60.degree. with respect
to the longitudinal direction of a ferromagnetic body having various
length l and width b. The magnetization is calculated by an integral
equation method. In the case of a square (l/b=1) as shown in FIG. 7A, the
direction of the magnetization M and the direction of the external
magnetic field He are identical. As l/b is increased, as shown in FIG. 7B,
FIG. 7C and FIG. 7D, the direction of the magnetization M is shifted
toward the longitudinal direction.
FIG. 8A, FIG. 8B and FIG. 8C are vector representation of the distribution
of magnetization of a ferromagnetic body of l/b=10, resulting from
application of all external magnetic field lie at various angles
.theta.=0.degree., 30.degree. and 60.degree. . The magnetization is
calculated by an integral equation method. As will be seen, when l/b is
large, i.e., when the ferromagnetic body is more elongated, the
magnetization M is in the longitudinal direction regardless of the
direction of the external magnetic field He applied. This is called a
shape effect, which is an anisotropy due to the elongated shape of the
magnetization of magnetic bodies. The apparent permeability .mu.', a
demagnetizing factor N and the permeability .mu. of the magnetic body of a
given shape are related as follows:
.mu.'=1/(1/.mu.+N/4.pi.) (3)
In an elongated flat magnetic body, the demagnetizing factor Nl in the
longitudinal direction is sufficiently smaller than the demagnetizing
factor Nb in the width direction, i.e.,
Nl<<Nb
Accordingly, the apparent permeability .mu.' in the longitudinal direction
is sufficiently larger than the apparent permeability .mu.b in the width
direction, i.e.,
.mu.'l>>.mu.'b
Accordingly, the longitudinal direction is the direction of easy
magnetization. Where the magnetic body is made of pure iron, the principal
component of magnetization is in the longitudinal direction, i.e., the
magnetization tend to be concentrated in the longitudinal direction if l/b
is 3 or more, unless the magnetic field is perpendicular to the
longitudinal direction, and when l/b>20, there is essentially no
magnetization other than in the longitudinal direction.
FIG. 9A to FIG. 9C are vector representation of the induced magnetic field
around one end (left end) of a strip-shaped magnetic body 0.1 cm thick, 1
cm wide and 10 cm long, when a magnetic field is applied in the horizontal
direction (side-to-side direction in the figures) . In FIG. 9A, the
strip-shaped magnetic body is straight and disposed to extend in the
horizontal direction. In FIG. 9B and FIG. 9C, the elongated sheet-shaped
magnetic body has a bent end, with the trunk portion extending
horizontally. Since the length is much greater than the thickness, because
of the shape effect, the magnetization M is along the length of the
magnetic body. An induced magnetic field is created around the tip (left
end). In the case of FIG. 9C, the direction of the induced magnetic lines
of force are mainly in the Y direction (vertical direction). That is, when
an elongated magnetic body is magnetized by an external magnetic field, it
is magnetized according to the shape of the body, and creates an induced
magnetic field around it. If this characteristic is utilized, the control
over the magnetic field distribution is possible.
Solid (black) circles, triangles and inverted triangles in FIG. 6 show Bx,
By and Bz obtained by measurements similar to those described above (in
connection with the blank circle, triangle and inverted triangle), but
with the magnetic shield MS comprising the J-shaped strips 10. It will be
observed by comparison with the blank circles, triangles and inverted
triangles that Bz is reduced, By is increased within the range of Z=0 to
200 mm, and the magnetic field distribution has thus been changed. The
miss-landing amount of the electron beam 9 at the corner part of the
phosphor screen as obtained by calculation of the path of the electron
beam 9 in the magnetic field is 77 .mu.m. This is much smaller than the
miss-landing amount (147 .mu.m) that results when the strips 10 are not
provided. Optimum designing can be achieved, in which the dimension and
disposition of the strips 10 so adjusted as to control the magnitude of
the induced magnetic field, and as to minimize the miss-landing amount due
to the magnetic field in the Z direction.
FIG. 10 shows the results of measurements similar to the measurements whose
results are shown in FIG. 6. The difference is that the external magnetic
filed in applied in the X direction, rather than in the Z direction. The
blank circles, triangles, and inverted triangles indicate the results
obtained when the shield MS is not provided, and the solid circles,
triangles and inverted triangles indicate the results obtained when the
shield MS is provided. In both cases, the circles, triangles and inverted
triangles indicate Bx, By and Bz. It will be seen that presence of the
magnetic shield MS little affect the magnetic flux or its distribution.
This is because the strips 10 of the magnetic shield MS are not magnetized
by the application of a magnetic field in their width direction, and the
interval .alpha. between adjacent strips 10 provides a large magnetic
resistance against a magnetic field in the X direction, and no magnetic
closed circuit is formed.
If the magnetic shield 8 were not provided in the cathode ray tube shown
ill FIG. 11, the bending of the electron beam 9 due to the magnetic field
in the X direction is mainly in the Y direction, because of the Fleming's
law, and there will be no color contamination if the phosphor screen 3 is
of the stripe-type. In this state, however, when the magnetic field is
applied in the Z direction, the miss-landing is in the X direction,
resulting in color contamination. The internal magnetic shield 8 is
mounted for preventing such color contamination. The magnetic shield 8
also has certain shielding effect against the magnetic field in the X
direction, but it also has the effect of varying the magnetic field in the
tube, with the result that the magnetic shield 8 is better not provided
for the X direction magnetic field. It is therefore difficult to reduce
the color contamination due to the magnetic fields in both of the Z and X
directions.
In contrast, in the above embodiment, the J-shaped magnetic shields 10
having a sufficient length and disposed at an interval .alpha., give no or
little effect on the X direction environmental magnetic field, and exhibit
a shielding effect against the Z direction environmental magnetic field.
Moreover, the tip parts 10t of the strips 10 are bent so that the tips 10a
are directed toward the X-Z plane (where Y=0), as shown in FIG. 1, the
magnetic field in the Z direction is transformed into the magnetic field
in the Y direction, so that the effect of the Z direction environmental
magnetic field is further reduced.
Also known in the art is a modification of the conventional internal
magnetic shield 8 shown in FIG. 11, in which the end of the shield 8 on
the entrance side are bent in the direction of the tube axis in an attempt
to eliminate the effects of the environmental magnetic field in a specific
direction. This arrangement is effective when the environmental direction
is in the specific direction, but if the environmental direction is other
direction, the results were worse than if the shield is not provided. The
strips 10 shown in FIG. 1 are not associated with such a problem.
The range over which the parameter in designing the strips 10 can be varied
will now be discussed. The strips 10 are disposed on the periphery of the
shadow mask 4, each strip is formed of a magnetic body having one end
fixed to the frame 5, and having the other end situated nearer to the
electron gun 2. In order to exhibit the shape effect explained with
reference to FIG. 7, the ratio of the length l to the width b should be
not less than 2, and preferably not less than 3. Since such shape effect
is derived even from a single strip 10, a plurality of such strips 10 need
not be provided along the entire side or along the entire corner part of
the frame 5. However, in practice, a plurality of strips 10 need to be
provided along one side or along one corner because the shielding effect
is required over a certain area of the phosphor screen. The interval
.alpha. between the adjacent strips 10 should be substantially greater
than the thickness t (the dimension normal to the side wall side of the
frame 5). In general, the inequality .alpha./t>>3 should be satisfied.
In the embodiment of FIG. 1, Bz is transformed into By. This transformation
effect is eminent because, in addition to the extension of the strips in
the Z direction, the tip parts 10t are bent so that the tips 10a are
directed toward the X-Z plane (Y=0). To obtain this effect sufficiently,
the length of the strips 10 should be sufficiently larger than the
thickness, as was explained with reference to FIG. 9. In the embodiment
shown In FIG. 1, the relationship l/t.gtoreq.5 should be satisfied, and
preferably, l/t.gtoreq.10 should be satisfied. The relationship
l/b.gtoreq.2 should also be satisfied.
In the embodiment described, the tip part is curved smoothly. But the tip
part may be bent sharply, and results similar to those of the
above-described embodiment are obtained.
FIG. 2 is a perspective view showing the pertinent part of the color
cathode ray tube of another embodiment of the invention. The parts and
members identical to those in FIG. 1 are identified by the same reference
numerals and their description is omitted. The difference of this
embodiment from the embodiment of FIG. 1 is that strips 10 does not have
individual root parts 10r, and instead a common connecting part 11, which
may be considered as a common root part, and which is common to all the
strips 10 along each of the longer sides of the shadow mask, is provided
and fixed to the longer side wall 5c of the frame 5. Each strip 10
comprises a trunk part 10s and a curved tip part 10t , and front ends of
trunk parts 10s of strips 10 are continuous to a rear edge of the
connecting part 11.
All the strips 10 and the connecting part 11 along each longer wall 5c of
the frame 5 may be formed by blanking a single sheet.
This configuration has an advantage that the strips 10 are supported with a
greater mechanical strength. The relationships l/t.gtoreq.5, l/b.gtoreq.2
and .alpha./t.gtoreq.3 should also be satisfied.
FIG. 3 is a perspective view showing the pertinent part of the color
cathode ray tube of a further embodiment. FIG. 3A shows, in enlarged cross
section, part 3A in FIG. 3. The parts and members identical to those in
FIG. 2 are identified by the same reference numerals and their description
is omitted. The difference of this embodiment from the embodiment of FIG.
2 is that the strips 10 are at an angle of inclination .theta. with
respect to the longer side wall 5c which is normal to the Y axis, and the
strips 10 are straight, and are not bent in the middle. The front ends of
the strips 10 are continuous to the connecting part 11 with an angle of
inclination .theta..
According to the embodiment of FIG. 3 and FIG. 3A, the effect due to the
bent rear ends as explained with reference to FIG. 9B and FIG. 9C, is not
obtained, but because of the angle of inclination .theta. with respect to
the longer side wall side 5c of the frame 5, a similar effect (though with
a lesser extent) is obtained. Moreover, the effect due to the elongated
shape of the strips 10 as explained with reference to FIG. 8 is obtained.
Because of the angle of inclination, the strips extend along the tapered
funnel 1b so that the space inside the tube is fully utilized, while
maximizing the effect of the elongated shape of the strips 10. The
relationships l/t.gtoreq.5, l/b.gtoreq.2 and .alpha./t.gtoreq.3 should
also be satisfied.
In another embodiment, not illustrated, the structure is similar to the
embodiment of FIG. 3 and FIG. 3A, but strips 10 are not inclined but
parallel to the Z axis. When the funnel 1b is not tapered in the region
where the magnetic shield MS is provided, or when there is enough extra
space between the region over which the electron beam is deflected and the
inner surface of the funnel 1b , then the strips 10 may not be inclined
and parallel to the tube axis. Such a configuration does not have the
effect of enhancing the magnetic field in the Y direction, but it has the
effect of reducing or canceling the magnetic field in the Z axis.
FIG. 4 is a perspective view of a pertinent portion of a color cathode ray
tube of a further embodiment of the invention. In the figure, parts or
members identical to those in FIG. 2 are denoted by identical reference
numerals. The difference of this embodiment from the embodiment of FIG. 2
is that the tip parts 10t of the strips 10 are connected to each other by
a non-magnetic member 12 to provide mechanical reinforcement. By virtue of
the reinforcement, a slight impact or contact with other bodies during
manufacture will not cause vibration or deformation (bending) of the tip
parts 10t of the strips 10, so that the effects of the particular shape of
the strips are ensured.
In the embodiments described, the strips 10 are mounted to the longer wall
sides 5c of the frame 5. It is however possible to mount the strips 10 to
the shorter wall sides 5d . All the strips 10 may not be identical in
shape. What is essential is that each of the strips 10 satisfies the
conditions described above. In particular, in or near the corner of the
frame 5, the directions of the magnetic flux varies in a complex manner,
so that it may be advantageous to vary the shape of the individual strips
10 to cancel or utilize the magnetic flux at the position of each strip
10.
The phosphor screen 3 may not be the stripe-type, but may be of the
dot-type.
In the embodiments described, the frame 5 is generally formed of a material
thicker than the shadow mask 4 for the purpose of supporting and
reinforcing the shadow mask 4. In a small-sized color cathode ray tube, it
is possible to bend the sheet which forms the shadow mask 4 so that the
bent part will provide the functions of supporting and/or reinforcement.
The strips 10 may then be mounted to such bent part of the shadow mask 4
providing the function of the frame. The term "frame" in the appended
claims should therefore be construed to cover such part of the shadow mask
providing the function of the support and/or reinforcement.
As has been described, according to the invention, one ends of elongated
magnetic members of a high permeability is fixed, and the other end parts
are disposed nearer to the electron gun, and the end of each of said other
end parts forms a magnetic tip. Because of the effect of their elongated
shape, the strips are magnetized in one specific direction, and the effect
of the terrestrial magnetism or other environmental magnetic field in the
specific direction, can be suppressed efficiently, without giving adverse
effect in other, orthogonal direction, so that color contamination can be
fully suppressed, and the performance of the color cathode ray tube is
substantially improved. Moreover, the shielding effect in the E-W
direction and the shielding effect in the N-S direction can be changed
independently of each other. Accordingly, the designing is facilitated,
and the cost of production can be lowered.
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